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motivation – local systems in physics:
Hilbert spaces of gapped quantum ground states over classical parameter space of topological phases of matter
topological phases are
topological orders in phase are
topological orders in any phase are
in fragile crystalline phases: parameter space is crystal lattice couplings reflected in 1-electron Hamiltonians from a space , hence parameter space is
topological phases are
topological orders in phase are
topological orders in any phase are
functorial at least in diffeos of (modular functor)
for crystalline structure use equivariant maps
translate to TFT language
in experiment, such FQ(A)H systems are governed by two effective symmetries
supersymmetry
area-preserving diffeomorphisms ()
same as characteristic symmetries of super -branes
find geometric engineering on M-branes in SuGra
need global IR-completion where topological brane charges are determined
(no string folklore, but actual definitions and proofs)
compare IR completion of Maxwell: and use Deligne complex…
…
magnetized M5 @ A1
(Milne 2017, Propositions 3.24, 3.25). Let be an algebraically closed field. The categories of affine varieties and affine -algebras are anti-equivalent.
The following result particularizes the fundamental theorem on morphisms of schemes to prevarieties.
Milne 2017, Propositions 5.11. Let be an algebraically closed field. Let be an algebraic -prevariety. Let be an affine -algebra. Then we have the following natural bijection:
In other words, the maximal spectrum functor and the global sections functor, defined between the categories of affine -algebras and -prevarieties, are mutually right adjoint. Note that Milne states the result for quasi-compact varieties, but his proof applies in the general case and never uses quasi-compactness nor separation. Note that from we recover .
For additional information, look at this very related typing graph.
Last revised on July 7, 2026 at 07:37:35. See the history of this page for a list of all contributions to it.